In mathematics, specifically in category theory, an extranatural transformation is a generalization of the notion of natural transformation.
Definition
Let F : A × B o p × B → D {\displaystyle F:A\times B^{\mathrm {op} }\times B\rightarrow D} and G : A × C o p × C → D {\displaystyle G:A\times C^{\mathrm {op} }\times C\rightarrow D} be two functors of categories. A family η ( a , b , c ) : F ( a , b , b ) → G ( a , c , c ) {\displaystyle \eta (a,b,c):F(a,b,b)\rightarrow G(a,c,c)} is said to be natural in a and extranatural in b and c if the following holds:
- η ( − , b , c ) {\displaystyle \eta (-,b,c)} is a natural transformation (in the usual sense).
- (extranaturality in b) ∀ ( g : b → b ′ ) ∈ M o r B {\displaystyle \forall (g:b\rightarrow b^{\prime })\in \mathrm {Mor} \,B} , ∀ a ∈ A {\displaystyle \forall a\in A} , ∀ c ∈ C {\displaystyle \forall c\in C} the following diagram commutes
- (extranaturality in c) ∀ ( h : c → c ′ ) ∈ M o r C {\displaystyle \forall (h:c\rightarrow c^{\prime })\in \mathrm {Mor} \,C} , ∀ a ∈ A {\displaystyle \forall a\in A} , ∀ b ∈ B {\displaystyle \forall b\in B} the following diagram commutes
Properties
Extranatural transformations can be used to define wedges and thereby ends2 (dually co-wedges and co-ends), by setting F {\displaystyle F} (dually G {\displaystyle G} ) constant.
Extranatural transformations can be defined in terms of dinatural transformations, of which they are a special case.3
See also
External links
- extranatural+transformation at the nLab
References
Eilenberg and Kelly, A generalization of the functorial calculus, J. Algebra 3 366–375 (1966) /wiki/Samuel_Eilenberg ↩
Fosco Loregian, This is the (co)end, my only (co)friend, arXiv preprint [1] https://arxiv.org/abs/1501.02503 ↩
Fosco Loregian, This is the (co)end, my only (co)friend, arXiv preprint [1] https://arxiv.org/abs/1501.02503 ↩